CN110207822B - High sensitivity optical time delay estimation system, method and medium - Google Patents

High sensitivity optical time delay estimation system, method and medium Download PDF

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CN110207822B
CN110207822B CN201910458302.6A CN201910458302A CN110207822B CN 110207822 B CN110207822 B CN 110207822B CN 201910458302 A CN201910458302 A CN 201910458302A CN 110207822 B CN110207822 B CN 110207822B
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output light
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黄靖正
黄朝政
曾贵华
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Shanghai Jiao Tong University
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/42Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry
    • G01J3/427Dual wavelengths spectrometry
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J2003/283Investigating the spectrum computer-interfaced
    • G01J2003/2836Programming unit, i.e. source and date processing
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J3/00Spectrometry; Spectrophotometry; Monochromators; Measuring colours
    • G01J3/28Investigating the spectrum
    • G01J3/42Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry
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Abstract

The invention provides a high-sensitivity optical time delay estimation system, a method and a medium, comprising the following steps: the system comprises a light source module, a polarization state pre-modulation module, an optical time delay sensing module, a combined spectrum detection module and a data processing module; the light source module is used for generating an original light signal, and the central wavelength of the original light signal is recorded as lambda0(ii) a The polarization pre-modulation module is used for pre-modulating the polarization of an original optical signal to generate first output light; the optical time delay sensing module is used for loading an optical time delay value to be measured to the first output light to generate second output light; the polarization state post-selection module is used for projecting and decomposing the second output light according to the specified polarization state to generate two paths of output light, namely third output light and fourth output light. The invention adopts a method of 'joint bias weak value amplification', realizes the measurement of tiny quantity such as time delay with extremely high sensitivity, and also provides a high-sensitivity measurement scheme for other optical parameter estimation tasks.

Description

高灵敏度光学时延估计系统、方法及介质High sensitivity optical time delay estimation system, method and medium

技术领域technical field

本发明涉及对微小物理量的测量技术,具体地,涉及一种高灵敏度光学时延估计系统、方法及介质。尤其地,涉及基于联合弱值放大技术的光学时延估计系统,可应用于实现光学精密测量,如光学相干层析等,提高分辨率和探测灵敏度。The present invention relates to the measurement technology of tiny physical quantities, in particular, to a high-sensitivity optical time delay estimation system, method and medium. In particular, it relates to an optical time delay estimation system based on joint weak value amplification technology, which can be applied to realize optical precision measurement, such as optical coherence tomography, etc., to improve resolution and detection sensitivity.

背景技术Background technique

在精密测量领域,弱测量技术主要分为两类:弱值放大弱测量和联合弱测量。其中,弱值放大弱测量技术提出的比较早,并且这种技术目前已经得到了广泛的应用。但是不可避免的,这种技术也存在着一些缺陷,例如:In the field of precision measurement, weak measurement techniques are mainly divided into two categories: weak value amplification weak measurement and joint weak measurement. Among them, the weak value amplification weak measurement technology was proposed earlier, and this technology has been widely used. But inevitably, this technology also has some flaws, such as:

1、弱值放大弱测量利用弱耦合和后选择技术,将本来很微小的参量适当的放大到一个可观测量的位置,从而间接的对微小量进行测量,这种“放大”是以牺牲后选择光子数而得到的,也就是说,当后选择角度与前选择角度越接近垂直时,放大倍数就越大,但在探测器上接收到的光子数就越少,可以利用的信息量就越小。1. Weak value amplification Weak measurement uses weak coupling and post-selection technology to properly amplify the originally very small parameter to an observable position, so as to indirectly measure the small amount. This "amplification" is to choose after sacrifice That is to say, when the post-selection angle is closer to the perpendicular to the pre-selection angle, the magnification will be larger, but the number of photons received on the detector will be less, and the amount of information that can be used will be greater. Small.

2、在弱值放大弱测量中,放大倍数的计算依赖于后选择角度,虽然后选择角度可以事先已知,但是在实验中,一旦后选择偏振片发生扰动,后选择角度就会偏离真实值,那么,测量精度就会有偏差。2. In the weak measurement of weak value amplification, the calculation of the magnification depends on the post-selection angle. Although the post-selection angle can be known in advance, in the experiment, once the post-selection polarizer is disturbed, the post-selection angle will deviate from the true value. , then the measurement accuracy will be biased.

由以上的描述可知,弱值放大方案均存在一些难以克服的缺陷。近年来,有学者提出了基于联合弱测量的参量估计方法。这种方法建立在弱值放大弱测量基础之上,不同的是,联合弱测量将后选择之后的光分成两路,并且同时测量所有的光子,这样做就可以收集全部的光子信息,提高测量精度;另外,联合弱测量利用最大似然估计的后处理算法得到偏移量,这种方法可以在未知后选择参数的情况下同时估计出微小参量和后选择参数,这样,即便在实验条件下后选择参数不稳定,利用联合弱测量的方法也不会影响参数估计的精度。因此,联合弱测量可以有效的弥补弱值放大弱测量的缺陷。然而,联合弱测量方法也存在以下不足:It can be seen from the above description that the weak value amplification schemes all have some insurmountable defects. In recent years, some scholars have proposed a parameter estimation method based on joint weak measurement. This method is based on weak value amplification and weak measurement. The difference is that the combined weak measurement divides the light after the post-selection into two paths, and measures all photons at the same time. In this way, all photon information can be collected and the measurement can be improved. In addition, the joint weak measurement uses the post-processing algorithm of maximum likelihood estimation to obtain the offset. This method can estimate the small parameters and the post-selection parameters at the same time when the post-selection parameters are unknown. In this way, even under experimental conditions The post-selection parameters are not stable, and the method of joint weak measurement will not affect the accuracy of parameter estimation. Therefore, the combined weak measurement can effectively make up for the defect of weak value amplification of weak measurement. However, the joint weak measurement method also has the following shortcomings:

1)设置相同弱值放大倍数情况下,偏移量只有传统弱值放大方法的一半(灵敏度下降一半);1) When setting the same weak value magnification, the offset is only half of the traditional weak value amplification method (the sensitivity is reduced by half);

2)无法通过调制偏置相位获得更高的弱值放大倍数。2) Higher weak value magnification cannot be obtained by modulating the bias phase.

由此可见,弱值放大和联合弱测量两种已有的弱测量方案均存在固有不足。本发明提出了一种实现弱测量参量估值的新方法,可以将弱值放大和联合弱测量两种方案的优点有机结合,相互取长补短,既能克服弱值放大方案效率过低,又能解决联合弱测量方案放大倍数难以提升的问题,为使用实现高效率、高灵敏度的参量测量提供一种可靠的技术途径。It can be seen that the two existing weak measurement schemes, weak value amplification and joint weak measurement, have inherent shortcomings. The invention proposes a new method for realizing the estimation of weak measurement parameters, which can organically combine the advantages of the weak value amplification and the joint weak measurement, and learn from each other's strengths to complement each other, which can not only overcome the low efficiency of the weak value amplification scheme, but also solve the The problem that the magnification of the combined weak measurement scheme is difficult to increase provides a reliable technical approach for the use of high-efficiency and high-sensitivity parameter measurement.

专利文献CN107121207A(申请号:201610101252.2)公开了一种基于联合弱测量技术的时间延迟估计方法及系统,包括:光学模块、数据采集模块和数据处理模块;其中,所述光学模块用于依据联合弱测量参数估计算法估计时间延迟;所述数据采集模块用于控制光谱仪采集数据;所述数据处理模块用于对测量数据进行分析和处理,获得时间延迟的估计值。Patent document CN107121207A (application number: 201610101252.2) discloses a time delay estimation method and system based on joint weak measurement technology, including: an optical module, a data acquisition module and a data processing module; wherein, the optical module is used to The measurement parameter estimation algorithm estimates the time delay; the data acquisition module is used to control the spectrometer to collect data; the data processing module is used to analyze and process the measurement data to obtain an estimated value of the time delay.

发明内容SUMMARY OF THE INVENTION

针对现有技术中的缺陷,本发明的目的是提供一种高灵敏度光学时延估计系统、方法及介质。In view of the defects in the prior art, the purpose of the present invention is to provide a high-sensitivity optical time delay estimation system, method and medium.

根据本发明提供的一种高灵敏度光学时延估计系统,包括:光源模块、偏振态预调制模块、光学时延感知模块、联合谱探测模块以及数据处理模块;A high-sensitivity optical delay estimation system provided according to the present invention includes: a light source module, a polarization state pre-modulation module, an optical delay sensing module, a joint spectrum detection module and a data processing module;

所述光源模块用于产生原始光信号,其中心波长记为λ0The light source module is used to generate the original optical signal, and its center wavelength is denoted as λ 0 ;

所述偏振预调制模块用于将原始光信号的偏振作预调制,产生第一输出光;The polarization pre-modulation module is used to pre-modulate the polarization of the original optical signal to generate the first output light;

所述光学时延感知模块用于将待测光学时延值加载到第一输出光,产生第二输出光;The optical delay sensing module is used to load the optical delay value to be measured into the first output light to generate the second output light;

所述偏振态后选择模块用于将第二输出光按指定偏振态作投影分解,产生两路输出光,即第三输出光和第四输出光;The polarization state post-selection module is used to project and decompose the second output light according to the specified polarization state to generate two output lights, namely the third output light and the fourth output light;

所述联合谱探测模块用于对第三输出光和第四输出光同时进行谱探测,输出光谱信号;The joint spectrum detection module is used for performing spectrum detection on the third output light and the fourth output light at the same time, and outputting a spectrum signal;

所述数据处理模块采集、存储输出的光谱信号,并对采集到的光谱信号进行分析和处理,获得时间延迟的估计值。The data processing module collects and stores the output spectral signal, and analyzes and processes the collected spectral signal to obtain an estimated value of the time delay.

优选地,所述偏振预调制模块包括:线性偏振片(1)和第一四分之一波片(2),Preferably, the polarization pre-modulation module comprises: a linear polarizer (1) and a first quarter-wave plate (2),

所述偏振预调制模块:The polarization pre-modulation module:

使光源模块产生的原始光信号通过线性偏振片(1)和第一四分之一波片(2),产生第一输出光,所述的线性偏振片方向设置为与水平面呈第一预设夹角,所述四分之一波片方向设置为与线性偏振片方向呈

Figure GDA0002145350880000031
夹角,所述第一输出光的偏振状态记作前选择态,记号表达为:The original optical signal generated by the light source module is passed through the linear polarizer (1) and the first quarter-wave plate (2) to generate the first output light, and the direction of the linear polarizer is set to be a first preset with the horizontal plane The included angle, the direction of the quarter wave plate is set to be in the direction of the linear polarizer
Figure GDA0002145350880000031
The included angle, the polarization state of the first output light is denoted as the preselected state, and the symbol is expressed as:

Figure GDA0002145350880000032
Figure GDA0002145350880000032

其中,in,

Figure GDA0002145350880000033
表示前选择偏振态;
Figure GDA0002145350880000033
represents the preselected polarization state;

|H>、|V>分别表示水平偏振态、垂直偏振态;|H>, |V> represent the horizontal polarization state and the vertical polarization state, respectively;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

e-iCε表示调制相位值-Cε;e -iCε represents the modulation phase value -Cε;

eiCε表示调制相位值Cε;e iCε represents the modulation phase value Cε;

需要调制的相位值C由下式计算得出:The phase value C that needs to be modulated is calculated by:

Figure GDA0002145350880000034
Figure GDA0002145350880000034

其中,in,

ω表示光信号的角频率,ω represents the angular frequency of the optical signal,

ω0表示光信号角频率的平均值。ω 0 represents the average value of the angular frequency of the optical signal.

所述光学时延感知模块包括:索累-巴比涅补偿器(3);The optical time delay sensing module includes: a Sorey-Barbinet compensator (3);

所述光学时延感知模块:使第一输出光通过索累-巴比涅补偿器,产生第二输出光;The optical delay sensing module: the first output light is passed through a Sore-Barbinet compensator to generate the second output light;

所述索累-巴比涅补偿器的方向设置为与线性偏振片呈第二预设夹角,相比于第一输出光,第二输出光的水平偏振分量与竖直偏振分量之间增加了一段传播延迟,把该延迟记作τ。The direction of the Soleil-Barbinet compensator is set to form a second preset angle with the linear polarizer, and compared with the first output light, the horizontal polarization component and the vertical polarization component of the second output light are increased. There is a propagation delay, and this delay is recorded as τ.

优选地,所述偏振态后选择模块包括:第二四分之一波片(4)和偏振分束器(5);Preferably, the polarization state post-selection module includes: a second quarter-wave plate (4) and a polarization beam splitter (5);

所述偏振态后选择模块:将第二输出光通过第二个四分之一波片(4)和偏振分束器(5),产生两路输出光,即第三输出光和第四输出光;The polarization state post-selection module: passing the second output light through the second quarter-wave plate (4) and the polarization beam splitter (5) to generate two output lights, namely the third output light and the fourth output Light;

所述第二个四分之一波片方向设置为与线性偏振片呈第三预设夹角,所述偏振分束器极化方向设置为与线性偏振片呈第四预设夹角。The direction of the second quarter-wave plate is set to form a third preset angle with the linear polarizer, and the polarization direction of the polarization beam splitter is set to form a fourth preset angle to the linear polarizer.

优选地,所述联合谱探测模块包括:第一光纤准直器(6)、第二光纤准直器(7)和带光开关模块的光谱仪(8);Preferably, the combined spectrum detection module comprises: a first fiber collimator (6), a second fiber collimator (7) and a spectrometer (8) with an optical switch module;

所述联合谱探测模块:将所述偏振态后选择模块产生的两路输出光分别通过光纤耦合设备进入接至光谱仪的光纤,进而被光谱仪采集,获得光谱信息;The joint spectrum detection module: the two output lights generated by the polarization state post-selection module are respectively entered into the optical fiber connected to the spectrometer through the optical fiber coupling device, and then collected by the spectrometer to obtain spectral information;

光谱仪采集到透射光的光谱分布为:The spectral distribution of the transmitted light collected by the spectrometer is:

Figure GDA0002145350880000041
Figure GDA0002145350880000041

P1i)表示透射光信号光谱的波长分布;P 1i ) represents the wavelength distribution of the transmitted light signal spectrum;

P0i)表示初始光信号光谱的波长分布;P 0i ) represents the wavelength distribution of the initial optical signal spectrum;

λ0表示平均波长,由公式∑iP(λii计算λ 0 represents the average wavelength, calculated by the formula ∑ i P(λ ii

λi表示光谱仪可探测到的某一波长刻度值;λ i represents a certain wavelength scale value that can be detected by the spectrometer;

c表示真空中的光速;c is the speed of light in vacuum;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

τ表示光学时延;τ represents the optical time delay;

Aw1i)表示一个复数值,由下式计算得出:A w1i ) represents a complex value and is calculated by:

Figure GDA0002145350880000042
Figure GDA0002145350880000042

Im[Aw1i)]表示Aw1i)的虚部;Im[A w1i )] represents the imaginary part of A w1i );

光谱仪采集到反射光的光谱分布为:The spectral distribution of the reflected light collected by the spectrometer is:

Figure GDA0002145350880000043
Figure GDA0002145350880000043

P2i)表示反射光信号光谱的波长分布;P 2i ) represents the wavelength distribution of the reflected light signal spectrum;

Aw2i)表示表示一个复数值,由下式计算得出:A w2i ) represents a complex value and is calculated by:

Figure GDA0002145350880000044
Figure GDA0002145350880000044

Im[Aw2i)]表示Aw2i)的虚部。Im[A w2i )] represents the imaginary part of A w2i ).

优选地,所述数据处理模块采集并存储联合谱探测模块获得的光谱信息;Preferably, the data processing module collects and stores the spectral information obtained by the joint spectral detection module;

根据所述联合谱探测模块获得的光谱信息,定义并计算如下平均波长值:According to the spectral information obtained by the joint spectral detection module, the following average wavelength values are defined and calculated:

Figure GDA0002145350880000045
Figure GDA0002145350880000045

Figure GDA0002145350880000047
表示按测量数据计算得到的平均波长值;
Figure GDA0002145350880000047
Indicates the average wavelength value calculated according to the measurement data;

通过以下公式解算出时间延迟的估计值:An estimate of the time delay is solved by the following formula:

Figure GDA0002145350880000046
Figure GDA0002145350880000046

其中,in,

τ表示待测的光学时延,即时间延迟的估计值;τ represents the optical delay to be measured, that is, the estimated value of the time delay;

c表示真空中的光速;c is the speed of light in vacuum;

δλ表示波长偏移量,通过将平均波长值

Figure GDA0002145350880000055
减去输入光的初始波长值λ0得到。δλ represents the wavelength offset, by dividing the average wavelength value
Figure GDA0002145350880000055
It is obtained by subtracting the initial wavelength value λ 0 of the input light.

根据本发明提供的一种高灵敏度光学时延估计方法,包括:光源产生步骤、偏振态预调制步骤、光学时延感知步骤、联合谱探测步骤以及数据处理步骤;A high-sensitivity optical time delay estimation method provided according to the present invention includes: a light source generating step, a polarization state pre-modulation step, an optical time delay sensing step, a joint spectrum detection step, and a data processing step;

所述光源步骤用于产生原始光信号,其中心波长记为λ0The light source step is used to generate the original optical signal, and its central wavelength is denoted as λ 0 ;

所述偏振预调制步骤用于将原始光信号的偏振作预调制,产生第一输出光;The polarization pre-modulation step is used to pre-modulate the polarization of the original optical signal to generate the first output light;

所述光学时延感知步骤用于将待测光学时延值加载到第一输出光,产生第二输出光;The optical delay sensing step is used to load the optical delay value to be measured into the first output light to generate the second output light;

所述偏振态后选择步骤用于将第二输出光按指定偏振态作投影分解,产生两路输出光,即第三输出光和第四输出光;The post-polarization state selection step is used to project and decompose the second output light according to the specified polarization state to generate two output lights, namely the third output light and the fourth output light;

所述联合谱探测步骤用于对第三输出光和第四输出光同时进行谱探测,输出光谱信号;The joint spectral detection step is used to perform spectral detection on the third output light and the fourth output light simultaneously, and output a spectral signal;

所述数据处理步骤采集、存储输出的光谱信号,并对采集到的光谱信号进行分析和处理,获得时间延迟的估计值。The data processing step collects and stores the output spectral signal, and analyzes and processes the collected spectral signal to obtain an estimated value of the time delay.

优选地,所述偏振预调制步骤:Preferably, the polarization pre-modulation step:

使光源产生步骤产生的原始光信号通过线性偏振片(1)和第一四分之一波片(2),产生第一输出光,所述的线性偏振片方向设置为与水平面呈第一预设夹角,所述四分之一波片方向设置为与线性偏振片方向呈

Figure GDA0002145350880000051
夹角,所述第一输出光的偏振状态记作前选择态,记号表达为:The original optical signal generated by the light source generating step is passed through the linear polarizer (1) and the first quarter-wave plate (2) to generate the first output light, and the direction of the linear polarizer is set to be in a first pre-position with the horizontal plane. Set the angle, the direction of the quarter wave plate is set to be in the direction of the linear polarizer.
Figure GDA0002145350880000051
The included angle, the polarization state of the first output light is denoted as the preselected state, and the symbol is expressed as:

Figure GDA0002145350880000052
Figure GDA0002145350880000052

其中,in,

Figure GDA0002145350880000053
表示前选择偏振态;
Figure GDA0002145350880000053
represents the preselected polarization state;

|H>、|V>分别表示水平偏振态、垂直偏振态;|H>, |V> represent the horizontal polarization state and the vertical polarization state, respectively;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

e-iCε表示调制相位值-C;e -iCε represents the modulation phase value -C;

eiCε表示调制相位值C;e iCε represents the modulation phase value C;

需要调制的相位值C由下式计算得出:The phase value C that needs to be modulated is calculated by:

Figure GDA0002145350880000054
Figure GDA0002145350880000054

其中,in,

ω表示光信号的角频率,ω represents the angular frequency of the optical signal,

ω0表示光信号角频率的平均值;ω 0 represents the average value of the angular frequency of the optical signal;

所述光学时延感知步骤:使第一输出光通过索累-巴比涅补偿器(3),产生第二输出光;The optical time delay sensing step: making the first output light pass through the Soleil-Barbinet compensator (3) to generate the second output light;

所述索累-巴比涅补偿器的方向设置为与线性偏振片呈第二预设夹角,相比于第一输出光,第二输出光的水平偏振分量与竖直偏振分量之间增加了一段传播延迟,把该延迟记作τ。The direction of the Soleil-Barbinet compensator is set to form a second preset angle with the linear polarizer, and compared with the first output light, the horizontal polarization component and the vertical polarization component of the second output light are increased. There is a propagation delay, and this delay is recorded as τ.

优选地,所述偏振态后选择步骤:将第二输出光通过第二个四分之一波片(4)和偏振分束器(5),产生两路输出光,即第三输出光和第四输出光;Preferably, the polarization state post-selection step: passing the second output light through the second quarter-wave plate (4) and the polarization beam splitter (5) to generate two output lights, namely the third output light and the the fourth output light;

所述第二个四分之一波片方向设置为与线性偏振片呈第三预设夹角,所述偏振分束器极化方向设置为与线性偏振片呈第四预设夹角;The direction of the second quarter wave plate is set to form a third preset angle with the linear polarizer, and the polarization direction of the polarization beam splitter is set to form a fourth preset angle with the linear polarizer;

所述联合谱探测步骤:将所述偏振态后选择步骤产生的两路输出光分别通过光纤耦合设备进入接至光谱仪的光纤,进而被光谱仪采集,获得光谱信息;The joint spectrum detection step: the two output lights generated by the polarization state post-selection step are respectively entered into the optical fiber connected to the spectrometer through the optical fiber coupling device, and then collected by the spectrometer to obtain spectral information;

光谱仪采集到透射光的光谱分布为:The spectral distribution of the transmitted light collected by the spectrometer is:

Figure GDA0002145350880000061
Figure GDA0002145350880000061

P1i)表示透射光信号光谱的波长分布;P 1i ) represents the wavelength distribution of the transmitted light signal spectrum;

P0i)表示初始光信号光谱的波长分布;P 0i ) represents the wavelength distribution of the initial optical signal spectrum;

λ0表示平均波长,由公式∑iP(λii计算λ 0 represents the average wavelength, calculated by the formula ∑ i P(λ ii

λi表示光谱仪可探测到的某一波长刻度值;λ i represents a certain wavelength scale value that can be detected by the spectrometer;

c表示真空中的光速;c is the speed of light in vacuum;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

τ表示光学时延;τ represents the optical time delay;

Aw1i)表示一个复数值,由下式计算得出:A w1i ) represents a complex value and is calculated by:

Figure GDA0002145350880000062
Figure GDA0002145350880000062

Im[Aw1i)]表示Aw1i)的虚部;Im[A w1i )] represents the imaginary part of A w1i );

光谱仪采集到反射光的光谱分布为:The spectral distribution of the reflected light collected by the spectrometer is:

Figure GDA0002145350880000063
Figure GDA0002145350880000063

P2i)表示反射光信号光谱的波长分布;P 2i ) represents the wavelength distribution of the reflected light signal spectrum;

Aw2i)表示表示一个复数值,由下式计算得出:A w2i ) represents a complex value and is calculated by:

Figure GDA0002145350880000071
Figure GDA0002145350880000071

Im[Aw2i)]表示Aw2i)的虚部。Im[A w2i )] represents the imaginary part of A w2i ).

优选地,所述数据处理步骤采集并存储联合谱探测步骤获得的光谱信息;Preferably, the data processing step collects and stores the spectral information obtained in the joint spectral detection step;

根据所述联合谱探测步骤获得的光谱信息,定义并计算如下平均波长值:According to the spectral information obtained by the joint spectral detection step, the following average wavelength values are defined and calculated:

Figure GDA0002145350880000072
Figure GDA0002145350880000072

Figure GDA0002145350880000075
表示按测量数据计算得到的平均波长值;
Figure GDA0002145350880000075
Indicates the average wavelength value calculated according to the measurement data;

通过以下公式解算出时间延迟的估计值:An estimate of the time delay is solved by the following formula:

Figure GDA0002145350880000073
Figure GDA0002145350880000073

其中,in,

τ表示待测的光学时延,即时间延迟的估计值;τ represents the optical delay to be measured, that is, the estimated value of the time delay;

c表示真空中的光速;c is the speed of light in vacuum;

δλ表示波长偏移量,通过将平均波长值

Figure GDA0002145350880000074
减去输入光的初始波长值λ0得到。δλ represents the wavelength offset, by dividing the average wavelength value
Figure GDA0002145350880000074
It is obtained by subtracting the initial wavelength value λ 0 of the input light.

根据本发明提供的一种存储有计算机程序的计算机可读存储介质,其特征在于,所述计算机程序被处理器执行时实现上述中任一项所述的高灵敏度光学时延估计方法的步骤。A computer-readable storage medium storing a computer program according to the present invention is characterized in that, when the computer program is executed by a processor, the steps of any one of the above-mentioned high-sensitivity optical time delay estimation methods are implemented.

与现有技术相比,本发明具有如下的有益效果:Compared with the prior art, the present invention has the following beneficial effects:

1、本发明可以将弱值放大和联合弱测量两种方案的优点有机结合,相互取长补短,既能克服弱值放大方案效率过低,又能解决联合弱测量方案放大倍数难以提升的问题,为使用实现高效率、高灵敏度的参量测量提供了一种可靠的技术途径。1. The present invention can organically combine the advantages of the weak value amplification and the joint weak measurement scheme, and learn from each other's strengths to complement each other, which can not only overcome the low efficiency of the weak value amplification scheme, but also solve the problem that the combined weak measurement scheme is difficult to increase the magnification. The use of high-efficiency, high-sensitivity parametric measurements provides a reliable technical approach.

2、本发明采用“联合偏置弱值放大”的方法,实现了对如时间延迟的微小量的极高灵敏度的测量,也为其他光学参量估值任务提供了一种高灵敏度的测量方案。2. The method of "joint bias weak value amplification" is adopted in the present invention, which realizes extremely sensitive measurement of minute quantities such as time delay, and also provides a highly sensitive measurement scheme for other optical parameter estimation tasks.

附图说明Description of drawings

通过阅读参照以下附图对非限制性实施例所作的详细描述,本发明的其它特征、目的和优点将会变得更明显:Other features, objects and advantages of the present invention will become more apparent by reading the detailed description of non-limiting embodiments with reference to the following drawings:

图1为本发明提供的基于联合弱测量的时间延迟结构示意图;1 is a schematic diagram of a time delay structure based on joint weak measurement provided by the present invention;

图2为本发明提供的高斯分布光信号的初始频谱示意图;2 is a schematic diagram of an initial spectrum of a Gaussian distributed optical signal provided by the present invention;

图3为本发明提供的非高斯分布光信号的初始频谱示意图;3 is a schematic diagram of an initial spectrum of a non-Gaussian distributed optical signal provided by the present invention;

图4为本发明提供的高斯分布光源模拟得到的频谱偏移率示意图;4 is a schematic diagram of a spectral shift rate obtained by simulation of a Gaussian distributed light source provided by the present invention;

图5为本发明提供的高斯分布光源模拟得到的频谱偏移率局部放大示意图;Fig. 5 is the partial enlarged schematic diagram of the spectral shift rate obtained by the simulation of the Gaussian distributed light source provided by the present invention;

图6为本发明提供的非高斯分布光源模拟得到的频谱偏移率;Fig. 6 is the spectral shift rate obtained by the simulation of the non-Gaussian distribution light source provided by the present invention;

图7为本发明提供的非高斯分布光源模拟得到的频谱偏移率局部放大示意图。FIG. 7 is a partially enlarged schematic diagram of the spectral shift rate obtained by the simulation of the non-Gaussian distribution light source provided by the present invention.

图中示出:The figure shows:

Figure GDA0002145350880000081
Figure GDA0002145350880000081

具体实施方式Detailed ways

下面结合具体实施例对本发明进行详细说明。以下实施例将有助于本领域的技术人员进一步理解本发明,但不以任何形式限制本发明。应当指出的是,对本领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干变化和改进。这些都属于本发明的保护范围。The present invention will be described in detail below with reference to specific embodiments. The following examples will help those skilled in the art to further understand the present invention, but do not limit the present invention in any form. It should be noted that, for those skilled in the art, several changes and improvements can be made without departing from the inventive concept. These all belong to the protection scope of the present invention.

根据本发明提供的一种高灵敏度光学时延估计系统,包括:光源模块、偏振态预调制模块、光学时延感知模块、联合谱探测模块以及数据处理模块;A high-sensitivity optical delay estimation system provided according to the present invention includes: a light source module, a polarization state pre-modulation module, an optical delay sensing module, a joint spectrum detection module and a data processing module;

所述光源模块用于产生原始光信号,其中心波长记为λ0The light source module is used to generate the original optical signal, and its center wavelength is denoted as λ 0 ;

所述偏振预调制模块用于将原始光信号的偏振作预调制,产生第一输出光;The polarization pre-modulation module is used to pre-modulate the polarization of the original optical signal to generate the first output light;

所述光学时延感知模块用于将待测光学时延值加载到第一输出光,产生第二输出光;The optical delay sensing module is used to load the optical delay value to be measured into the first output light to generate the second output light;

所述偏振态后选择模块用于将第二输出光按指定偏振态作投影分解,产生两路输出光,即第三输出光和第四输出光;The polarization state post-selection module is used to project and decompose the second output light according to the specified polarization state to generate two output lights, namely the third output light and the fourth output light;

所述联合谱探测模块用于对第三输出光和第四输出光同时进行谱探测,输出光谱信号;The joint spectrum detection module is used for performing spectrum detection on the third output light and the fourth output light at the same time, and outputting a spectrum signal;

所述数据处理模块采集、存储输出的光谱信号,并对采集到的光谱信号进行分析和处理,获得时间延迟的估计值。The data processing module collects and stores the output spectral signal, and analyzes and processes the collected spectral signal to obtain an estimated value of the time delay.

具体地,所述偏振预调制模块包括:线性偏振片(1)和第一四分之一波片(2),Specifically, the polarization pre-modulation module includes: a linear polarizer (1) and a first quarter-wave plate (2),

所述偏振预调制模块:The polarization pre-modulation module:

使光源模块产生的原始光信号通过线性偏振片(1)和第一四分之一波片(2),产生第一输出光,所述的线性偏振片方向设置为与水平面呈第一预设夹角,所述四分之一波片方向设置为与线性偏振片方向呈

Figure GDA0002145350880000091
夹角,所述第一输出光的偏振状态记作前选择态,记号表达为:The original optical signal generated by the light source module is passed through the linear polarizer (1) and the first quarter-wave plate (2) to generate the first output light, and the direction of the linear polarizer is set to be a first preset with the horizontal plane The included angle, the direction of the quarter wave plate is set to be in the direction of the linear polarizer
Figure GDA0002145350880000091
The included angle, the polarization state of the first output light is denoted as the preselected state, and the symbol is expressed as:

Figure GDA0002145350880000092
Figure GDA0002145350880000092

其中,in,

Figure GDA0002145350880000093
表示前选择偏振态;
Figure GDA0002145350880000093
represents the preselected polarization state;

|H>、|V>分别表示水平偏振态、垂直偏振态;|H>, |V> represent the horizontal polarization state and the vertical polarization state, respectively;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

e-iCε表示调制相位值-Cε;e -iCε represents the modulation phase value -Cε;

eiCε表示调制相位值Cε;e iCε represents the modulation phase value Cε;

需要调制的相位值C由下式计算得出:The phase value C that needs to be modulated is calculated by:

Figure GDA0002145350880000094
Figure GDA0002145350880000094

其中,in,

ω表示光信号的角频率,ω represents the angular frequency of the optical signal,

ω0表示光信号角频率的平均值。ω 0 represents the average value of the angular frequency of the optical signal.

所述光学时延感知模块包括:索累-巴比涅补偿器(3);The optical time delay sensing module includes: a Sorey-Barbinet compensator (3);

所述光学时延感知模块:使第一输出光通过索累-巴比涅补偿器,产生第二输出光;the optical time delay sensing module: the first output light is passed through a Soleil-Barbinet compensator to generate the second output light;

所述索累-巴比涅补偿器的方向设置为与线性偏振片呈第二预设夹角,相比于第一输出光,第二输出光的水平偏振分量与竖直偏振分量之间增加了一段传播延迟,把该延迟记作τ。The direction of the Soleil-Barbinet compensator is set to form a second preset angle with the linear polarizer, and compared with the first output light, the horizontal polarization component and the vertical polarization component of the second output light are increased. There is a propagation delay, and this delay is recorded as τ.

具体地,所述偏振态后选择模块包括:第二四分之一波片(4)和偏振分束器(5);Specifically, the polarization state post-selection module includes: a second quarter-wave plate (4) and a polarization beam splitter (5);

所述偏振态后选择模块:将第二输出光通过第二个四分之一波片(4)和偏振分束器(5),产生两路输出光,即第三输出光和第四输出光;The polarization state post-selection module: passing the second output light through the second quarter-wave plate (4) and the polarization beam splitter (5) to generate two output lights, namely the third output light and the fourth output Light;

所述第二个四分之一波片方向设置为与线性偏振片呈第三预设夹角,所述偏振分束器极化方向设置为与线性偏振片呈第四预设夹角。The direction of the second quarter-wave plate is set to form a third preset angle with the linear polarizer, and the polarization direction of the polarization beam splitter is set to form a fourth preset angle to the linear polarizer.

具体地,所述联合谱探测模块包括:第一光纤准直器(6)、第二光纤准直器(7)和带光开关模块的光谱仪(8);Specifically, the combined spectrum detection module includes: a first fiber collimator (6), a second fiber collimator (7), and a spectrometer (8) with an optical switch module;

所述联合谱探测模块:将所述偏振态后选择模块产生的两路输出光分别通过光纤耦合设备进入接至光谱仪的光纤,进而被光谱仪采集,获得光谱信息;The joint spectrum detection module: the two output lights generated by the polarization state post-selection module are respectively entered into the optical fiber connected to the spectrometer through the optical fiber coupling device, and then collected by the spectrometer to obtain spectral information;

光谱仪采集到透射光的光谱分布为:The spectral distribution of the transmitted light collected by the spectrometer is:

Figure GDA0002145350880000101
Figure GDA0002145350880000101

P1i)表示透射光信号光谱的波长分布;P 1i ) represents the wavelength distribution of the transmitted light signal spectrum;

P0i)表示初始光信号光谱的波长分布;P 0i ) represents the wavelength distribution of the initial optical signal spectrum;

λ0表示平均波长,由公式∑iP(λii计算λ 0 represents the average wavelength, calculated by the formula ∑ i P(λ ii

λi表示光谱仪可探测到的某一波长刻度值;λ i represents a certain wavelength scale value that can be detected by the spectrometer;

c表示真空中的光速;c is the speed of light in vacuum;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

τ表示光学时延;τ represents the optical time delay;

Aw1i)表示一个复数值,由下式计算得出:A w1i ) represents a complex value and is calculated by:

Figure GDA0002145350880000102
Figure GDA0002145350880000102

Im[Aw1i)]表示Aw1i)的虚部;Im[A w1i )] represents the imaginary part of A w1i );

光谱仪采集到反射光的光谱分布为:The spectral distribution of the reflected light collected by the spectrometer is:

Figure GDA0002145350880000103
Figure GDA0002145350880000103

P2i)表示反射光信号光谱的波长分布;P 2i ) represents the wavelength distribution of the reflected light signal spectrum;

Aw2i)表示表示一个复数值,由下式计算得出:A w2i ) represents a complex value and is calculated by:

Figure GDA0002145350880000104
Figure GDA0002145350880000104

Im[Aw2i)]表示Aw2i)的虚部。Im[A w2i )] represents the imaginary part of A w2i ).

具体地,所述数据处理模块采集并存储联合谱探测模块获得的光谱信息;Specifically, the data processing module collects and stores the spectral information obtained by the joint spectral detection module;

根据所述联合谱探测模块获得的光谱信息,定义并计算如下平均波长值:According to the spectral information obtained by the joint spectral detection module, the following average wavelength values are defined and calculated:

Figure GDA0002145350880000105
Figure GDA0002145350880000105

Figure GDA0002145350880000107
表示按测量数据计算得到的平均波长值;
Figure GDA0002145350880000107
Indicates the average wavelength value calculated according to the measurement data;

通过以下公式解算出时间延迟的估计值:An estimate of the time delay is solved by the following formula:

Figure GDA0002145350880000106
Figure GDA0002145350880000106

其中,in,

τ表示待测的光学时延,即时间延迟的估计值;τ represents the optical delay to be measured, that is, the estimated value of the time delay;

c表示真空中的光速;c is the speed of light in vacuum;

δλ表示波长偏移量,通过将平均波长值

Figure GDA0002145350880000111
减去输入光的初始波长值λ0得到。δλ represents the wavelength offset, by dividing the average wavelength value
Figure GDA0002145350880000111
It is obtained by subtracting the initial wavelength value λ 0 of the input light.

本发明提供的高灵敏度光学时延估计系统,可以通过本发明给的高灵敏度光学时延估计方法的步骤流程实现。本领域技术人员可以将所述高灵敏度光学时延估计方法,理解为所述高灵敏度光学时延估计系统的一个优选例。The high-sensitivity optical time delay estimation system provided by the present invention can be realized through the steps of the high-sensitivity optical time delay estimation method provided by the present invention. Those skilled in the art can understand the high-sensitivity optical time delay estimation method as a preferred example of the high-sensitivity optical time delay estimation system.

根据本发明提供的一种高灵敏度光学时延估计方法,包括:光源产生步骤、偏振态预调制步骤、光学时延感知步骤、联合谱探测步骤以及数据处理步骤;According to a high-sensitivity optical time delay estimation method provided by the present invention, the method includes: a light source generating step, a polarization state pre-modulation step, an optical time delay sensing step, a joint spectrum detection step, and a data processing step;

所述光源步骤用于产生原始光信号,其中心波长记为λ0The light source step is used to generate the original optical signal, and its central wavelength is denoted as λ 0 ;

所述偏振预调制步骤用于将原始光信号的偏振作预调制,产生第一输出光;The polarization pre-modulation step is used to pre-modulate the polarization of the original optical signal to generate the first output light;

所述光学时延感知步骤用于将待测光学时延值加载到第一输出光,产生第二输出光;The optical delay sensing step is used to load the optical delay value to be measured into the first output light to generate the second output light;

所述偏振态后选择步骤用于将第二输出光按指定偏振态作投影分解,产生两路输出光,即第三输出光和第四输出光;The post-polarization state selection step is used to project and decompose the second output light according to the specified polarization state to generate two output lights, namely the third output light and the fourth output light;

所述联合谱探测步骤用于对第三输出光和第四输出光同时进行谱探测,输出光谱信号;The joint spectral detection step is used to perform spectral detection on the third output light and the fourth output light simultaneously, and output a spectral signal;

所述数据处理步骤采集、存储输出的光谱信号,并对采集到的光谱信号进行分析和处理,获得时间延迟的估计值。The data processing step collects and stores the output spectral signal, and analyzes and processes the collected spectral signal to obtain an estimated value of the time delay.

具体地,所述偏振预调制步骤:Specifically, the polarization pre-modulation step:

使光源产生步骤产生的原始光信号通过线性偏振片(1)和第一四分之一波片(2),产生第一输出光,所述的线性偏振片方向设置为与水平面呈第一预设夹角,所述四分之一波片方向设置为与线性偏振片方向呈

Figure GDA0002145350880000112
夹角,所述第一输出光的偏振状态记作前选择态,记号表达为:The original optical signal generated by the light source generating step is passed through the linear polarizer (1) and the first quarter-wave plate (2) to generate the first output light, and the direction of the linear polarizer is set to be in a first pre-position with the horizontal plane. Set the angle, the direction of the quarter wave plate is set to be in the direction of the linear polarizer.
Figure GDA0002145350880000112
The included angle, the polarization state of the first output light is denoted as the preselected state, and the symbol is expressed as:

Figure GDA0002145350880000113
Figure GDA0002145350880000113

其中,in,

Figure GDA0002145350880000114
表示前选择偏振态;
Figure GDA0002145350880000114
represents the preselected polarization state;

|H>、|V>分别表示水平偏振态、垂直偏振态;|H>, |V> represent the horizontal polarization state and the vertical polarization state, respectively;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

e-iCε表示调制相位值-C;e -iCε represents the modulation phase value -C;

eiCε表示调制相位值C;e iCε represents the modulation phase value C;

需要调制的相位值C由下式计算得出:The phase value C that needs to be modulated is calculated by:

Figure GDA0002145350880000115
Figure GDA0002145350880000115

其中,in,

ω表示光信号的角频率,ω represents the angular frequency of the optical signal,

ω0表示光信号角频率的平均值;ω 0 represents the average value of the angular frequency of the optical signal;

所述光学时延感知步骤:使第一输出光通过索累-巴比涅补偿器(3),产生第二输出光;The optical time delay sensing step: making the first output light pass through the Soleil-Barbinet compensator (3) to generate the second output light;

所述索累-巴比涅补偿器的方向设置为与线性偏振片呈第二预设夹角,相比于第一输出光,第二输出光的水平偏振分量与竖直偏振分量之间增加了一段传播延迟,把该延迟记作τ。The direction of the Soleil-Barbinet compensator is set to form a second preset angle with the linear polarizer, and compared with the first output light, the horizontal polarization component and the vertical polarization component of the second output light are increased. There is a propagation delay, and this delay is recorded as τ.

具体地,所述偏振态后选择步骤:将第二输出光通过第二个四分之一波片(4)和偏振分束器(5),产生两路输出光,即第三输出光和第四输出光;Specifically, the polarization state post-selection step: passing the second output light through the second quarter-wave plate (4) and the polarization beam splitter (5) to generate two output lights, namely the third output light and the the fourth output light;

所述第二个四分之一波片方向设置为与线性偏振片呈第三预设夹角,所述偏振分束器极化方向设置为与线性偏振片呈第四预设夹角;The direction of the second quarter wave plate is set to form a third preset angle with the linear polarizer, and the polarization direction of the polarization beam splitter is set to form a fourth preset angle with the linear polarizer;

所述联合谱探测步骤:将所述偏振态后选择步骤产生的两路输出光分别通过光纤耦合设备进入接至光谱仪的光纤,进而被光谱仪采集,获得光谱信息;The joint spectrum detection step: the two output lights generated by the polarization state post-selection step are respectively entered into the optical fiber connected to the spectrometer through the optical fiber coupling device, and then collected by the spectrometer to obtain spectral information;

光谱仪采集到透射光的光谱分布为:The spectral distribution of the transmitted light collected by the spectrometer is:

Figure GDA0002145350880000121
Figure GDA0002145350880000121

P1i)表示透射光信号光谱的波长分布;P 1i ) represents the wavelength distribution of the transmitted light signal spectrum;

P0i)表示初始光信号光谱的波长分布;P 0i ) represents the wavelength distribution of the initial optical signal spectrum;

λ0表示平均波长,由公式∑iP(λii计算λ 0 represents the average wavelength, calculated by the formula ∑ i P(λ ii

λi表示光谱仪可探测到的某一波长刻度值;λ i represents a certain wavelength scale value that can be detected by the spectrometer;

c表示真空中的光速;c is the speed of light in vacuum;

ε表示一个远小于1的实数值;ε represents a real value much less than 1;

τ表示光学时延;τ represents the optical time delay;

Aw1i)表示一个复数值,由下式计算得出:A w1i ) represents a complex value and is calculated by:

Figure GDA0002145350880000122
Figure GDA0002145350880000122

Im[Aw1i)]表示Aw1i)的虚部;Im[A w1i )] represents the imaginary part of A w1i );

光谱仪采集到反射光的光谱分布为:The spectral distribution of the reflected light collected by the spectrometer is:

Figure GDA0002145350880000123
Figure GDA0002145350880000123

P2i)表示反射光信号光谱的波长分布;P 2i ) represents the wavelength distribution of the reflected light signal spectrum;

Aw2i)表示表示一个复数值,由下式计算得出:A w2i ) represents a complex value and is calculated by:

Figure GDA0002145350880000131
Figure GDA0002145350880000131

Im[Aw2i)]表示Aw2i)的虚部。Im[A w2i )] represents the imaginary part of A w2i ).

具体地,所述数据处理步骤采集并存储联合谱探测步骤获得的光谱信息;Specifically, the data processing step collects and stores the spectral information obtained by the joint spectral detection step;

根据所述联合谱探测步骤获得的光谱信息,定义并计算如下平均波长值:According to the spectral information obtained by the joint spectral detection step, the following average wavelength values are defined and calculated:

Figure GDA0002145350880000132
Figure GDA0002145350880000132

Figure GDA0002145350880000133
表示按测量数据计算得到的平均波长值;
Figure GDA0002145350880000133
Indicates the average wavelength value calculated according to the measurement data;

通过以下公式解算出时间延迟的估计值:An estimate of the time delay is solved by the following formula:

Figure GDA0002145350880000134
Figure GDA0002145350880000134

其中,in,

τ表示待测的光学时延,即时间延迟的估计值;τ represents the optical delay to be measured, that is, the estimated value of the time delay;

c表示真空中的光速;c is the speed of light in vacuum;

δλ表示波长偏移量,通过将平均波长值

Figure GDA0002145350880000135
减去输入光的初始波长值λ0得到。δλ represents the wavelength offset, by dividing the average wavelength value
Figure GDA0002145350880000135
It is obtained by subtracting the initial wavelength value λ 0 of the input light.

根据本发明提供的一种存储有计算机程序的计算机可读存储介质,其特征在于,所述计算机程序被处理器执行时实现上述中任一项所述的高灵敏度光学时延估计方法的步骤。A computer-readable storage medium storing a computer program according to the present invention is characterized in that, when the computer program is executed by a processor, the steps of any one of the above-mentioned high-sensitivity optical time delay estimation methods are implemented.

下面通过优选例,对本发明进行更为具体地说明。Hereinafter, the present invention will be described in more detail through preferred examples.

优选例1:Preferred Example 1:

根据本发明提供的具有极高灵敏度的联合弱值放大新方法,应用上述任一项所述的基于联合弱测量技术的时间延迟估计系统;包括如下步骤:According to the new method for joint weak value amplification with extremely high sensitivity provided by the present invention, the time delay estimation system based on the joint weak measurement technique described in any one of the above is applied; including the following steps:

偏振预调制和光学时延感知步骤:对光源发出的光进行处理,获得与待测参量相关的反射光和透射光信号光谱;Polarization pre-modulation and optical time delay sensing steps: process the light emitted by the light source to obtain the reflected light and transmitted light signal spectra related to the parameters to be measured;

偏振态后选择步骤:用于将光信号按指定偏振态作投影分解;Post-polarization selection step: used to project and decompose the optical signal according to the specified polarization state;

联合谱探测步骤:用于对两路输出光信号同时进行谱探测;Joint spectral detection step: used to perform spectral detection on two output optical signals at the same time;

数据采集和处理步骤:控制光谱信号采集的进程,实现光谱信号的采集和存储;对数据采集步骤中采集到的光谱信号进行分析和处理,获得时间延迟的估计值。Data acquisition and processing steps: control the process of spectral signal acquisition to realize the acquisition and storage of spectral signals; analyze and process the spectral signals collected in the data acquisition step to obtain an estimated value of time delay.

优选地,所述偏振预调制和光学时延感知步骤包括:Preferably, the polarization pre-modulation and optical delay sensing steps include:

步骤A1:对光源信号光进行偏振态前选择。具体为,使超辐射发光二极管光源发出的光通过线性偏振片和四分之一波片,产生输出光。所述的线性偏振片方向设置为与水平面呈45°夹角,所述四分之一波片方向设置为与线性偏振片方向呈

Figure GDA0002145350880000141
夹角,输出光的偏振状态记作前选择态,记号表达为:Step A1: Pre-selecting the polarization state of the light source signal light. Specifically, the light emitted by the superluminescent light emitting diode light source is passed through the linear polarizer and the quarter-wave plate to generate output light. The direction of the linear polarizer is set at an angle of 45° with the horizontal plane, and the direction of the quarter wave plate is set at an angle of 45° with the direction of the linear polarizer.
Figure GDA0002145350880000141
The included angle, the polarization state of the output light is recorded as the preselected state, and the notation is expressed as:

Figure GDA0002145350880000142
Figure GDA0002145350880000142

其中,

Figure GDA0002145350880000143
记号
Figure GDA0002145350880000144
表示前选择态,|H>和|V>分别表示水平偏振和垂直偏振态;in,
Figure GDA0002145350880000143
mark
Figure GDA0002145350880000144
represents the preselected state, |H> and |V> represent the horizontal and vertical polarization states, respectively;

步骤A2:产生弱耦合。具体为,使前选择态的光通过索累-巴比涅补偿器,产生输出光。所述索累-巴比涅补偿器的方向设置为与线性偏振片呈45°夹角。相比于输入光,输出光的水平偏振分量与竖直偏振分量之间增加了一段传播延迟,把该延迟记作τStep A2: Generate weak coupling. Specifically, the light in the preselected state is passed through a Soleil-Barbinet compensator to generate output light. The direction of the Sore-Barbinet compensator is set to form an included angle of 45° with the linear polarizer. Compared with the input light, a propagation delay is added between the horizontal polarization component and the vertical polarization component of the output light, and this delay is recorded as τ

优选地,所述偏振态后选择步骤包括:Preferably, the post-selecting step of the polarization state includes:

步骤B:对前一步骤输出的光信号进行偏振态后选择。具体为,将上一步骤输出的光信号通过第二个四分之一波片和偏振分束器,产生两路输出光。所述第二个四分之一波片方向设置为与线性偏振片呈45°夹角,所述偏振分束器极化方向设置为与线性偏振片呈0°夹角。输出的两路光分别记为透射光和反射光。Step B: After selecting the polarization state of the optical signal output in the previous step. Specifically, the optical signal output in the previous step is passed through the second quarter-wave plate and the polarization beam splitter to generate two output lights. The direction of the second quarter wave plate is set at an angle of 45° with the linear polarizer, and the polarization direction of the polarization beam splitter is set at an angle of 0° with the linear polarizer. The two output lights are respectively recorded as transmitted light and reflected light.

优选地,联合谱探测步骤包括:Preferably, the joint spectrum detection step includes:

步骤C:联合弱测量过程。具体为,将上一步骤产生的两路输出光分别通过光纤耦合设备进入接至光谱仪的光纤,进而被光谱仪采集。Step C: Joint Weak Measurement Process. Specifically, the two output lights generated in the previous step are respectively entered into the optical fiber connected to the spectrometer through the optical fiber coupling device, and then collected by the spectrometer.

光谱仪采集到透射光的光谱分布为:The spectral distribution of the transmitted light collected by the spectrometer is:

Figure GDA0002145350880000145
Figure GDA0002145350880000145

光谱仪采集到反射光的光谱分布为:The spectral distribution of the reflected light collected by the spectrometer is:

Figure GDA0002145350880000146
Figure GDA0002145350880000146

式中,弱值放大倍数Aw1(λ)和Aw2(λ)由下式定义:where the weak value magnifications A w1 (λ) and A w2 (λ) are defined by:

Figure GDA0002145350880000147
Figure GDA0002145350880000147

优选地,所述数据采集和处理步骤包括:Preferably, the data collection and processing steps include:

步骤D1:通过IP网络将计算机与光开关、光谱分析仪连接;Step D1: connect the computer with the optical switch and the spectrum analyzer through the IP network;

步骤D2:通过调用动态链接库函数,在Labview平台或FPGA上实现与光开关和光谱分析仪之间的串口通信。在此基础上编写程序控制光谱分析仪的参数设置,控制光开关的切换和光谱分析仪数据的采集。将采集到的光谱数据和光谱分析仪内置分析功能输出数据保存为文件。Step D2: realize serial communication with the optical switch and the spectrum analyzer on the Labview platform or FPGA by calling the dynamic link library function. On this basis, a program is written to control the parameter setting of the spectrum analyzer, control the switching of the optical switch and the acquisition of the spectrum analyzer data. Save the collected spectral data and the output data of the built-in analysis function of the spectrum analyzer as a file.

步骤D3:根据步骤C所得的光强分布,采用最大似然估计方法得到时间延迟的估计值。具体地,根据数据采集步骤所得的光强分布,定义并计算如下平均波长值:Step D3: According to the light intensity distribution obtained in Step C, the maximum likelihood estimation method is used to obtain the estimated value of the time delay. Specifically, according to the light intensity distribution obtained in the data collection step, the following average wavelength values are defined and calculated:

Figure GDA0002145350880000151
Figure GDA0002145350880000151

然后,利用如下公式计算待估计的时延值:Then, use the following formula to calculate the delay value to be estimated:

Figure GDA0002145350880000152
Figure GDA0002145350880000152

式中,τ表示待测的光学时延,c表示真空中的光速,δλ表示波长偏移量,通过将步骤C计算得到的平均波长值

Figure GDA0002145350880000153
减去输入光的初始波长值λ0得到。In the formula, τ represents the optical time delay to be measured, c represents the speed of light in vacuum, δλ represents the wavelength offset, and the average wavelength value calculated by step C is
Figure GDA0002145350880000153
It is obtained by subtracting the initial wavelength value λ 0 of the input light.

优选例2:Preferred example 2:

本发明提供的基于联合弱值放大技术的参量估计方法及其在高精度光学时延检测中的应用方案,采用偏置前选择、联合测量和计算平均波长偏移值的方法获得未知参量。The parameter estimation method based on the joint weak value amplification technology and its application scheme in high-precision optical time delay detection provided by the invention adopt the methods of pre-bias selection, joint measurement and calculation of the average wavelength offset value to obtain unknown parameters.

在本实施例中,本发明提供的具有极高灵敏度的微小延迟测量系统,包括:光学模块、数据采集模块和数据处理模块;其中,所述光学模块用于对信号源发出的光进行相应处理,获得该信号源对应的透射光和反射光的光谱;所述数据采集模块用于控制光学模块,实现光谱信号的采集并保存;所述数据处理模块用于对数据采集模块采集到的光谱信号进行分析和处理,获得时间延迟的估计值。In this embodiment, the micro-delay measurement system with extremely high sensitivity provided by the present invention includes: an optical module, a data acquisition module and a data processing module; wherein the optical module is used for corresponding processing of the light emitted by the signal source , obtain the spectrum of the transmitted light and reflected light corresponding to the signal source; the data acquisition module is used to control the optical module to realize the collection and storage of spectral signals; the data processing module is used to collect the spectral signals collected by the data acquisition module Analysis and processing are performed to obtain an estimate of the time delay.

所述光学模块用于产生时间延迟的具体过程如下:The specific process of the optical module for generating the time delay is as follows:

如图1所示,激光源为SLD光源,中心波长在1540nm,线宽25nm。经过起偏器后变成线偏振光,起偏器可以选用格兰泰勒棱镜。而后光束经过第一四分之一波片,波片与起偏器呈如上所述的夹角,完成前选择阶段。As shown in Figure 1, the laser source is an SLD light source with a central wavelength of 1540 nm and a line width of 25 nm. After passing through a polarizer, it becomes linearly polarized light, and the polarizer can be a Glan-Taylor prism. The beam then passes through the first quarter-wave plate, which forms an angle with the polarizer as described above, completing the pre-selection stage.

在实验中,系统的初始态为In the experiment, the initial state of the system is

Figure GDA0002145350880000154
Figure GDA0002145350880000154

其中,

Figure GDA0002145350880000155
为前选择态,|H>和|V>分别为水平极化和垂直极化态。in,
Figure GDA0002145350880000155
is the preselected state, and |H> and |V> are the horizontally and vertically polarized states, respectively.

当光束经过前选择后,入射到一个主轴垂直于水平面的双折射晶体中,当这个双折射晶体以光轴为轴向,逆时针旋转一定的角度θ时,前选择光水平极化分量和垂直极化分量之间会有一个非常微弱的时间延迟,可以表示为After the light beam is preselected, it is incident on a birefringent crystal whose main axis is perpendicular to the horizontal plane. When the birefringent crystal takes the optical axis as the axial direction and rotates counterclockwise by a certain angle θ, the horizontal polarization component of the preselected light and the vertical There will be a very weak time delay between the polarization components, which can be expressed as

Figure GDA0002145350880000161
Figure GDA0002145350880000161

其中,ne,no和n分别为e光、o光和平均折射率,c为光速,λ为入射光频率。Among them, n e , n o and n are e light, o light and the average refractive index, respectively, c is the speed of light, and λ is the frequency of the incident light.

上式建立了时间延迟τ和倾斜角度θ的关系,在实验中控制双折射晶体的倾斜角度就可以得到不同的时间延迟。The above formula establishes the relationship between the time delay τ and the tilt angle θ. Different time delays can be obtained by controlling the tilt angle of the birefringent crystal in the experiment.

时间延迟产生后,光束经过第二四分之一波片和一个极化偏振片(PBS),光经过PBS后分成两路,被光谱仪接收。其中四分之一波片被调至与起偏器呈45°夹角,偏振分束器极化光轴的指向被调至与起偏器相同。结合波片的方向设置使得在零偏置时两个光谱仪接收到的光强近似相等,满足联合弱测量的设计。After the time delay is generated, the light beam passes through a second quarter-wave plate and a polarizing polarizer (PBS). The quarter-wave plate is adjusted to form an angle of 45° with the polarizer, and the polarization axis of the polarization beam splitter is adjusted to the same direction as the polarizer. Combined with the direction setting of the wave plate, the light intensities received by the two spectrometers are approximately equal at zero offset, which satisfies the design of joint weak measurement.

实例中,经过后选择后,两个方向的后选择态分别为In the example, after post-selection, the post-selection states of the two directions are

Figure GDA0002145350880000162
Figure GDA0002145350880000162

Figure GDA0002145350880000163
Figure GDA0002145350880000163

其中,

Figure GDA0002145350880000164
Figure GDA0002145350880000165
分别为透射光和反射光的后选择态,φ为偏振分束器的极化角度。经过后选择后,两路光的弱值分别记为Aw1、Aw2,计算公式如下:in,
Figure GDA0002145350880000164
and
Figure GDA0002145350880000165
are the post-selected states of transmitted light and reflected light, respectively, and φ is the polarization angle of the polarizing beam splitter. After post-selection, the weak values of the two paths of light are recorded as A w1 and A w2 respectively, and the calculation formula is as follows:

Figure GDA0002145350880000166
Figure GDA0002145350880000166

经过后选择后,两束光的光子被探测到的概率在频谱上的分布为:After post-selection, the distribution of the probability of the photons of the two beams of light being detected on the spectrum is:

Figure GDA0002145350880000167
Figure GDA0002145350880000167

Figure GDA0002145350880000168
Figure GDA0002145350880000168

Figure GDA0002145350880000169
Figure GDA0002145350880000169

Figure GDA00021453508800001610
Figure GDA00021453508800001610

其中P1(ω)和P2(ω)分别表示两路光的光谱,P0(ω)=|f0(ω)|2是光束的初始光谱,其平均值为ω0where P 1 (ω) and P 2 (ω) represent the spectra of the two beams, respectively, and P 0 (ω)=|f 0 (ω)| 2 is the initial spectrum of the light beam, and its average value is ω 0 .

所述数据采集模块的具体过程如下:The specific process of the data acquisition module is as follows:

这套基于LABVIEW或FPGA的数据采集系统能够控制光谱仪和光开关从而对光谱数据进行采集。首先用路由器等设备将计算机与光开关、光谱分析仪稳固连接,启动计算机、光开关和光谱分析仪。在Labview程序中通过观察串口是否显示出光开关、光谱分析仪的名称,判断与计算机串口通信是否正常。由编写的Labview程序发送命令向光谱分析仪传入设置,并扫描光谱,程序同时控制光开关切换配合光谱分析仪分别接收从偏振分束器输出的两路光。本实例中对光谱分析仪的主要设置为:500采样点、HIGH1灵敏度、自动电平、采样中心为1577nm且扫描宽度为100nm。程序通过串口获取从光谱分析仪回馈的光谱数据和内置分析功能输出数据,然后将其保存在文件中。This LABVIEW or FPGA-based data acquisition system can control the spectrometer and optical switch to collect spectral data. First, use routers and other equipment to connect the computer firmly to the optical switch and spectrum analyzer, and start the computer, optical switch, and spectrum analyzer. In the Labview program, judge whether the communication with the computer serial port is normal by observing whether the serial port displays the name of the optical switch and the spectrum analyzer. The Labview program written by the program sends commands to the spectrum analyzer to input the settings and scans the spectrum. The program simultaneously controls the switching of the optical switch and cooperates with the spectrum analyzer to receive the two paths of light output from the polarization beam splitter. The main settings for the spectrum analyzer in this example are: 500 sampling points, HIGH1 sensitivity, auto level, sampling center at 1577 nm and scan width at 100 nm. The program obtains the spectral data fed back from the spectrum analyzer and the output data of the built-in analysis function through the serial port, and then saves it in a file.

所述数据处理模块具体过程如下:通过编写代码对采集的数据进行处理。在实例中,当我们获取了两路光的频谱分布函数,就可以通过上述算法来估计出当光经过光学时延模块后横截面水平分量和垂直分量之间在传播方向上的待测时间延迟τ值。从文件中读取光谱数据,依照如下公式计算平均波长:The specific process of the data processing module is as follows: the collected data is processed by writing codes. In the example, when we obtain the spectral distribution functions of the two paths of light, the above algorithm can be used to estimate the time delay to be measured in the propagation direction between the horizontal component and the vertical component of the cross-section after the light passes through the optical delay module. τ value. Read the spectral data from the file and calculate the average wavelength according to the following formula:

Figure GDA0002145350880000171
Figure GDA0002145350880000171

式中,P1i)和P2i)分别表示接收到的两路光的光谱强度,λi表示光谱分析仪对波长的每一个采样点。In the formula, P 1i ) and P 2i ) represent the spectral intensities of the received two paths of light respectively, and λ i represents each sampling point of the wavelength by the spectrum analyzer.

然后可以如下公式解算出光学时延值:Then the optical delay value can be calculated as follows:

Figure GDA0002145350880000172
Figure GDA0002145350880000172

式中,τ表示待测的光学时延,c表示真空中的光速,δλ表示波长偏移量,通过将计算得到的平均波长值

Figure GDA0002145350880000173
减去输入光的初始平均波长值λ0得到,λ0依光源特性不同而变化,在实例中由光谱分析仪测定。In the formula, τ represents the optical time delay to be measured, c represents the speed of light in vacuum, δλ represents the wavelength offset, and the average wavelength value obtained by calculating
Figure GDA0002145350880000173
It is obtained by subtracting the initial average wavelength value λ 0 of the input light, which varies with the characteristics of the light source and is measured by a spectrum analyzer in the example.

优选例3:Preferred example 3:

根据本发明提供的基于联合弱值放大的极高灵敏度光学时延估计系统,其特征在于,包括光源模块、偏振态预调制模块、光学时延感知模块、联合谱探测模块以及数据处理模块,其中:The extremely high sensitivity optical delay estimation system based on joint weak value amplification provided according to the present invention is characterized by comprising a light source module, a polarization state premodulation module, an optical delay sensing module, a joint spectrum detection module and a data processing module, wherein :

1、所述光源模块包括超辐射发光二极管,用于产生原始光信号。1. The light source module includes a superluminescent light emitting diode, which is used to generate the original light signal.

具体地,超辐射发光二极管产生高功率宽带光束,其中心波长记为λ0Specifically, the superluminescent light-emitting diode generates a high-power broadband beam, the central wavelength of which is denoted as λ 0 ;

2、所述偏振预调制模块包括线性偏振片和第一四分之一波片,用于将信号光偏振作预调制;2. The polarization pre-modulation module includes a linear polarizer and a first quarter-wave plate for pre-modulating the polarization of the signal light;

具体地,原始光信号通过设置在特定角度的线性偏振片和第一四分之一波片,输出前选择偏振态的光束。Specifically, the original optical signal passes through the linear polarizer and the first quarter-wave plate set at a specific angle, and outputs a beam of previously selected polarization state.

3、所述光学时延感知模块包括索累-巴比涅补偿器,用于将待测光学时延值加载到信号光;3. The optical delay sensing module includes a Soleil-Barbinet compensator, which is used to load the optical delay value to be measured into the signal light;

具体地,前选择偏振态的光束通过索累-巴比涅补偿器,输出带有时延信息的光束。Specifically, the light beam with the preselected polarization state passes through a Sorey-Barbinet compensator, and outputs a light beam with time delay information.

4、所述偏振态后选择模块包括第二四分之一波片和偏振分束器,用于将光信号按指定偏振态作投影分解;4. The polarization state post-selection module includes a second quarter-wave plate and a polarization beam splitter, which is used to project and decompose the optical signal according to the specified polarization state;

具体地,带有时延信息的光束通过设置在特定角度的第二四分之一波片和偏振分束器,输出两束偏振态相互垂直的光束。Specifically, the light beam with time delay information passes through a second quarter-wave plate and a polarization beam splitter arranged at a specific angle, and outputs two light beams with mutually perpendicular polarization states.

5、所述联合谱探测模块包括光纤准直器、光纤、光开关和光谱分析仪,用于对两路输出光信号同时进行谱探测;5. The joint spectrum detection module includes an optical fiber collimator, an optical fiber, an optical switch and a spectrum analyzer, which is used to perform spectrum detection on the two output optical signals at the same time;

具体地,分束器的两路输出光分别通过光纤准直器和光纤,进入光开关,然后进入光谱分析仪。Specifically, the two output lights of the beam splitter pass through the fiber collimator and the fiber respectively, enter the optical switch, and then enter the spectrum analyzer.

6、所述数据处理模块包括基于Labview或FPGA和Matlab的平台软件系统,实现光谱信号的采集、存储并对采集到的光谱信号进行分析和处理,获得时间延迟的估计值。6. The data processing module includes a platform software system based on Labview or FPGA and Matlab, realizes the collection and storage of spectral signals, analyzes and processes the collected spectral signals, and obtains an estimated value of time delay.

具体地,通过IP协议与光开关、光谱分析仪通信的Labview平台发送控制命令,控制光开关的切换、光谱分析仪的设置、光谱数据和光谱分析仪内置分析功能输出数据的采集,并将采集到的信息存储为文件。Matlab或其他语言编写的程序对文件内的数据进行处理,得出时延的估计值。Specifically, the Labview platform that communicates with the optical switch and the spectrum analyzer through the IP protocol sends control commands to control the switching of the optical switch, the setting of the spectrum analyzer, the collection of spectral data and the output data of the built-in analysis function of the spectrum analyzer, and the collection of The received information is stored as a file. Programs written in Matlab or other languages process the data in the file to obtain an estimate of the delay.

光谱分析仪的分析结果如图2至图7所示。The analysis results of the spectrum analyzer are shown in Figures 2 to 7.

本领域技术人员知道,除了以纯计算机可读程序代码方式实现本发明提供的系统及其各个装置以外,完全可以通过将方法步骤进行逻辑编程来使得本发明提供的系统及其各个装置以逻辑门、开关、专用集成电路、可编程逻辑控制器以及嵌入式微控制器等的形式来实现相同功能。所以,本发明提供的系统及其各项装置可以被认为是一种硬件部件,对其包括的用于实现各种功能的装置,可以视为硬件部件内的结构,也可以视为实现方法的软件模块。Those skilled in the art know that, in addition to implementing the system provided by the present invention and its respective devices in the form of pure computer-readable program codes, the system provided by the present invention and its respective devices can be made by logic gates, Switches, application-specific integrated circuits, programmable logic controllers, and embedded microcontrollers are used to achieve the same function. Therefore, the system provided by the present invention and its various devices can be regarded as a hardware component, and the devices included in it for realizing various functions can be regarded as the structure in the hardware component, and can also be regarded as the implementation method. software module.

以上对本发明的具体实施例进行了描述。需要理解的是,本发明并不局限于上述特定实施方式,本领域技术人员可以在权利要求的范围内做出各种变化或修改,这并不影响本发明的实质内容。在不冲突的情况下,本申请的实施例和实施例中的特征可以任意相互组合。Specific embodiments of the present invention have been described above. It should be understood that the present invention is not limited to the above-mentioned specific embodiments, and those skilled in the art can make various changes or modifications within the scope of the claims, which do not affect the essential content of the present invention. The embodiments of the present application and features in the embodiments may be combined with each other arbitrarily, provided that there is no conflict.

Claims (8)

1. A high-sensitivity optical time delay estimation system, comprising: the system comprises a light source module, a polarization state pre-modulation module, an optical time delay sensing module, a combined spectrum detection module, a data processing module and a polarization state post-selection module;
the light source module is used for generating an original light signal, and the central wavelength of the original light signal is recorded as lambda0
The polarization state pre-modulation module is used for pre-modulating the polarization of an original optical signal to generate first output light;
the optical time delay sensing module is used for loading an optical time delay value to be measured to the first output light to generate second output light;
the polarization state post-selection module is used for performing projection decomposition on the second output light according to a specified polarization state to generate two paths of output light, namely third output light and fourth output light;
the combined spectrum detection module is used for simultaneously performing spectrum detection on the third output light and the fourth output light and outputting a spectrum signal;
the data processing module collects and stores the output spectrum signals, analyzes and processes the collected spectrum signals and obtains an estimated value of optical time delay;
the combined spectrum detection module comprises: a first optical fiber collimator (6), a second optical fiber collimator (7) and a spectrometer (8) with an optical switch module;
the combined spectrum detection module: the two paths of output light generated by the selection module after polarization state enter optical fibers connected with a spectrometer through optical fiber coupling equipment respectively and are further collected by the spectrometer to obtain spectral information;
the spectral distribution of the transmitted light collected by the spectrometer is:
Figure FDA0002486677510000011
P1i) A wavelength distribution representing a spectrum of the transmitted light signal;
P0i) A wavelength distribution representing the spectrum of the original optical signal;
λ0expressing the initial average wavelength value, represented by formula ∑iP(λiiComputing
λiA scale value of a certain wavelength which can be detected by a spectrometer;
c represents the speed of light in vacuum;
represents a real number much less than 1;
τ represents the optical time delay;
Aw1i) Represents a complex value, calculated by:
Figure FDA0002486677510000021
Im[Aw1i)]is represented by Aw1i) An imaginary part of (d);
the spectral distribution of the reflected light collected by the spectrometer is as follows:
Figure FDA0002486677510000022
P2i) Representing the wavelength of the spectrum of the reflected light signalDistributing;
Aw2i) Represents a complex value, calculated by:
Figure FDA0002486677510000023
Im[Aw2i)]is represented by Aw2i) The imaginary part of (c).
2. The high-sensitivity optical time delay estimation system of claim 1, wherein the polarization state pre-modulation module comprises: a linear polarizer (1) and a first quarter-wave plate (2),
the polarization state pre-modulation module:
the method comprises the steps that an original light signal generated by a light source module passes through a linear polarizer (1) and a first quarter-wave plate (2) to generate first output light, the direction of the linear polarizer is set to form a first preset included angle with a horizontal plane, and the direction of the first quarter-wave plate is set to form a first preset included angle with the direction of the linear polarizer
Figure FDA0002486677510000024
An angle, the polarization state of the first output light being recorded as a pre-selected polarization state, the notation being:
Figure FDA0002486677510000025
wherein,
Figure FDA0002486677510000026
representing a pre-selected polarization state;
i H > and I V > respectively represent a horizontal polarization state and a vertical polarization state;
represents a real number much less than 1;
e-iCrepresents the modulation phase value-C;
eiCrepresents the modulation phase value C;
the phase value C to be modulated is calculated by:
Figure FDA0002486677510000027
wherein,
ω represents the angular frequency of the optical signal,
ω0an average value representing the angular frequency of the optical signal;
the optical time delay perception module comprises: a Sory-Babinet compensator (3);
the optical time delay perception module: making the first output light pass through a Sorri-Babinet compensator to generate a second output light;
the direction of the Sorrill-Babinet compensator is set to form a second preset included angle with the linear polaroid, compared with the first output light, a section of propagation optical time delay is added between the horizontal polarization component and the vertical polarization component of the second output light, and the optical time delay is recorded as tau.
3. The high-sensitivity optical time delay estimation system of claim 1, wherein the polarization post-selection module comprises: a second quarter wave plate (4) and a polarizing beam splitter (5);
the polarization state post-selection module: the second output light passes through a second quarter-wave plate (4) and a polarization beam splitter (5) to generate two paths of output light, namely third output light and fourth output light;
the second quarter-wave plate (4) is arranged to form a third preset included angle with the linear polaroid, and the polarization direction of the polarization beam splitter is arranged to form a fourth preset included angle with the linear polaroid.
4. The high-sensitivity optical time delay estimation system of claim 1, wherein the data processing module collects and stores spectral information obtained by the combined spectrum detection module;
according to the spectrum information obtained by the combined spectrum detection module, the following average wavelength value is defined and calculated:
Figure FDA0002486677510000031
Figure FDA0002486677510000032
represents the average wavelength value calculated from the measured data;
the estimated value of the time delay is solved by the following formula:
Figure FDA0002486677510000033
wherein,
tau represents the optical time delay to be measured, namely the estimated value of the time delay;
c represents the speed of light in vacuum;
λ represents the wavelength shift amount by averaging the wavelength values
Figure FDA0002486677510000034
Subtracting the initial average wavelength value lambda of the input light0Thus obtaining the product.
5. A method for high-sensitivity optical time delay estimation, comprising: the method comprises the steps of light source generation, polarization state pre-modulation, optical time delay perception, joint spectrum detection, data processing and polarization state post-selection;
the light source generating step is used for generating an original light signal, and the central wavelength of the original light signal is recorded as lambda0
The polarization state pre-modulation step is used for pre-modulating the polarization of the original optical signal to generate first output light;
the optical time delay sensing step is used for loading an optical time delay value to be measured to the first output light to generate second output light;
the polarization state post-selection step is used for performing projection decomposition on the second output light according to a specified polarization state to generate two paths of output light, namely third output light and fourth output light;
the combined spectrum detection step is used for simultaneously carrying out spectrum detection on the third output light and the fourth output light and outputting a spectrum signal;
the data processing step collects and stores the output spectrum signals, and analyzes and processes the collected spectrum signals to obtain an estimated value of optical time delay;
the polarization state post-selection step: the second output light passes through a second quarter-wave plate (4) and a polarization beam splitter (5) to generate two paths of output light, namely third output light and fourth output light;
the second quarter-wave plate is arranged to form a third preset included angle with the linear polarizer, and the polarization direction of the polarization beam splitter is arranged to form a fourth preset included angle with the linear polarizer;
the combined spectrum detection step comprises: the two paths of output light generated in the step of selecting after polarization state enter optical fibers connected with a spectrometer through optical fiber coupling equipment respectively and are further collected by the spectrometer to obtain spectral information;
the spectral distribution of the transmitted light collected by the spectrometer is:
Figure FDA0002486677510000041
P1i) A wavelength distribution representing a spectrum of the transmitted light signal;
P0i) A wavelength distribution representing the spectrum of the original optical signal;
λ0expressing the initial average wavelength value, represented by formula ∑iP(λiiComputing
λiA scale value of a certain wavelength which can be detected by a spectrometer;
c represents the speed of light in vacuum;
represents a real number much less than 1;
τ represents the optical time delay;
Aw1i) Represents a complex value, calculated by:
Figure FDA0002486677510000042
Im[Aw1i)]is represented by Aw1i) An imaginary part of (d);
the spectral distribution of the reflected light collected by the spectrometer is as follows:
Figure FDA0002486677510000043
P2i) A wavelength distribution representing a spectrum of the reflected light signal;
Aw2i) Represents a complex value, calculated by:
Figure FDA0002486677510000051
Im[Aw2i)]is represented by Aw2i) The imaginary part of (c).
6. The method according to claim 5, wherein the polarization pre-modulation step:
the original light signal generated in the light source generating step passes through a linear polaroid (1) and a first quarter-wave plate (2) to generate first output light, the direction of the linear polaroid is set to form a first preset included angle with the horizontal plane, and the direction of the first quarter-wave plate is set to form a first preset included angle with the direction of the linear polaroid
Figure FDA0002486677510000052
An angle, the polarization state of the first output light being recorded as a pre-selected polarization state, the notation being:
Figure FDA0002486677510000053
wherein,
Figure FDA0002486677510000054
representing a pre-selected polarization state;
i H > and I V > respectively represent a horizontal polarization state and a vertical polarization state;
represents a real number much less than 1;
e-iCrepresents the modulation phase value-C;
eiCrepresents the modulation phase value C;
the phase value C to be modulated is calculated by:
Figure FDA0002486677510000055
wherein,
ω represents the angular frequency of the optical signal,
ω0an average value representing the angular frequency of the optical signal;
the optical time delay sensing step: passing the first output light through a Sorri-Babinet compensator (3) to produce a second output light;
the direction of the Sorrill-Babinet compensator is set to form a second preset included angle with the linear polaroid, compared with the first output light, a section of propagation optical time delay is added between the horizontal polarization component and the vertical polarization component of the second output light, and the optical time delay is recorded as tau.
7. The high-sensitivity optical time delay estimation method according to claim 6, wherein the data processing step collects and stores the spectral information obtained by the combined spectrum detection step;
defining and calculating the following average wavelength values according to the spectrum information obtained in the combined spectrum detection step:
Figure FDA0002486677510000061
Figure FDA0002486677510000062
represents the average wavelength value calculated from the measured data;
the estimated value of the time delay is solved by the following formula:
Figure FDA0002486677510000063
wherein,
tau represents the optical time delay to be measured, namely the estimated value of the time delay;
c represents the speed of light in vacuum;
λ represents the wavelength shift amount by averaging the wavelength values
Figure FDA0002486677510000064
Subtracting the initial average wavelength value lambda of the input light0Thus obtaining the product.
8. A computer-readable storage medium storing a computer program, wherein the computer program, when executed by a processor, implements the steps of the high-sensitivity optical time delay estimation method of any one of claims 5 to 7.
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